CN107102298B - Radar Covariance Matrix Reconstruction Beamforming Method Based on Iterative Mutual Coupling Correction - Google Patents

Radar Covariance Matrix Reconstruction Beamforming Method Based on Iterative Mutual Coupling Correction Download PDF

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CN107102298B
CN107102298B CN201710510046.1A CN201710510046A CN107102298B CN 107102298 B CN107102298 B CN 107102298B CN 201710510046 A CN201710510046 A CN 201710510046A CN 107102298 B CN107102298 B CN 107102298B
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CN107102298A (en
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王彤
解彩莲
胡艳艳
李博文
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Xian University of Electronic Science and Technology
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Abstract

本发明公开了一种基于迭代互耦校正的雷达协方差矩阵重构波束形成方法,其思路为:确定均匀圆阵,该均匀圆阵包括M个阵元,均匀圆阵设定范围内存在Q个信号源,Q个信号源向均匀圆阵发射Q个入射信号,所述Q个入射信号包含1个期望信号和Q‑1个干扰信号;获取均匀圆阵的采样协方差矩阵R并进行特征分解,得到M个特征值;计算入射方向为(θ,φ)的信号MUSIC谱,然后设定均匀圆阵的互耦矩阵初始值,进而得到Q个入射信号的Q个方位角初始值,并分别得到均匀圆阵的最终互偶矩阵和Q个入射信号的最终方位角然后计算重构后均匀圆阵的干扰加噪声协方差矩阵进而得到均匀圆阵的自适应波束形成器的权矢量,完成了基于迭代互耦校正的均匀圆阵干扰加噪声协方差矩阵重构。

The invention discloses a radar covariance matrix reconstruction beamforming method based on iterative mutual coupling correction. The idea is to determine a uniform circular array, which includes M array elements, and there are Q signal sources, Q signal sources transmit Q incident signals to the uniform circular array, and the Q incident signals include 1 desired signal and Q-1 interference signals; obtain the sampling covariance matrix R of the uniform circular array and perform characterization Decompose to obtain M eigenvalues; calculate the MUSIC spectrum of the signal with the incident direction (θ, φ), and then set the initial value of the mutual coupling matrix of the uniform circular array, and then obtain the initial values of Q azimuth angles of the Q incident signals, and The final mutual dual matrix of the uniform circular array is obtained respectively and the final azimuths of the Q incident signals Then calculate the interference-plus-noise covariance matrix of the reconstructed uniform circular array Then the weight vector of the adaptive beamformer of the uniform circular array is obtained, and the reconstruction of the interference-plus-noise covariance matrix of the uniform circular array based on iterative mutual coupling correction is completed.

Description

基于迭代互耦校正的雷达协方差矩阵重构波束形成方法Radar Covariance Matrix Reconstruction Beamforming Method Based on Iterative Mutual Coupling Correction

技术领域technical field

本发明属于共形阵天线波束形成技术领域,特别涉及一种基于迭代互耦校正的雷达协方差矩阵重构波束形成方法,适用于解决采样样本中期望信号功率较强导致自适应波束形成器稳健性下降的问题,以及考虑互偶效应时波束形成器性能下降的问题,并且在考虑阵元间互耦效应的同时改善了波束形成器的稳健性能。The invention belongs to the technical field of conformal array antenna beamforming, and particularly relates to a radar covariance matrix reconstruction beamforming method based on iterative mutual coupling correction, which is suitable for solving the problem that the adaptive beamformer is robust due to the strong expected signal power in sampling samples The problem of performance degradation, and the performance degradation of the beamformer when considering the mutual coupling effect, and the robust performance of the beamformer is improved while considering the mutual coupling effect between array elements.

背景技术Background technique

共形阵列由于其具有电磁隐蔽性、大的扫描角度、小的负载重量及不干扰飞行体空气动力流场等优点而得到广泛的应用;然而,共形阵列波束形成技术在理论研究和开发应用方面都面临若干难题。首先,传统波束形成技术具有在实际环境中稳健性能不足的缺陷,这种缺陷应用到共形阵时依然存在;另外,阵列天线接收的信号在接收单元内部传输时,阵元间的互偶效应不容忽视。而共形阵复杂的阵元分布,加大了对其电磁特性进行精确分析和建模的难度,使得共形阵的互耦校正十分困难。故在充分发挥共形阵列优势的前提下,设计稳健的波束形成算法,突破互耦因素对波束形成器的限制是亟待解决的问题。Conformal arrays have been widely used due to their advantages of electromagnetic concealment, large scanning angle, small load weight, and no interference with the aerodynamic flow field of flying objects; however, conformal array beamforming technology is widely used in theoretical research and development applications face several difficulties. First of all, the traditional beamforming technology has the defect of insufficient robustness in the actual environment, which still exists when it is applied to the conformal array; in addition, when the signal received by the array antenna is transmitted inside the receiving unit, the mutual coupling effect between the array elements Can not be ignored. However, the complex element distribution of the conformal array increases the difficulty of accurate analysis and modeling of its electromagnetic characteristics, making the mutual coupling correction of the conformal array very difficult. Therefore, under the premise of giving full play to the advantages of conformal arrays, it is an urgent problem to design a robust beamforming algorithm and break through the limitations of mutual coupling factors on beamformers.

自适应波束形成技术的理论研究起始于20世纪60年代。1969年,Capon提出最小方差无失真响应(MVDR)准则,该准则在保证期望信号增益的同时最小化阵列的输出功率,为波束形成器抑制干扰提供了理论基础。20世纪70年代,研究人员提出了采样矩阵求逆(SMI)算法,该算法使用阵列接收信号快拍估计干扰加噪声协方差矩阵,能够自适应的抑制干扰信号。1974年,Brennan等人推导出了SMI波束形成算法的输出信干噪比的概率密度函数,给出了自适应算法的性能与训练样本数的关系。Theoretical research on adaptive beamforming technology began in the 1960s. In 1969, Capon proposed the Minimum Variance Distortionless Response (MVDR) criterion, which minimizes the output power of the array while ensuring the desired signal gain, and provides a theoretical basis for the beamformer to suppress interference. In the 1970s, researchers proposed the sampling matrix inversion (SMI) algorithm, which uses snapshots of array received signals to estimate the interference-plus-noise covariance matrix, which can adaptively suppress interference signals. In 1974, Brennan et al. derived the probability density function of the output signal-to-interference-noise ratio of the SMI beamforming algorithm, and gave the relationship between the performance of the adaptive algorithm and the number of training samples.

在众多实际应用领域中,自适应波束形成器的性能会受到各种误差因素的影响,如信号观测误差,接收通道误差,阵元位置误差等,这些误差会造成阵列天线接收信号导向矢量失配,导致波束形成算法性能下降;而且当样本快拍中含有期望信号时,导向矢量的失配对自适应波束形成器的性能影响尤为显著。In many practical application fields, the performance of the adaptive beamformer will be affected by various error factors, such as signal observation error, receiving channel error, array element position error, etc. These errors will cause the steering vector mismatch of the array antenna receiving signal , leading to the degradation of the performance of the beamforming algorithm; and when the sample snapshot contains the desired signal, the mismatch of the steering vector has a particularly significant impact on the performance of the adaptive beamformer.

在1991年,Benjamin Friedlander和W Anthony J.Weiss提出一种在阵元间存在互耦时的DOA估计方法,可以较为准确的估计出信号的波达方向DOA和均匀圆阵间的互耦,但是该在阵元间存在互耦时的DOA估计方法在自适应波束形成技术领域没有应用;在2012年,Gu提出了一种基于干扰加噪声协方差矩阵重构的波束形成方法,该方法利用重构后的协方差矩阵代替受到期望污染采样协方差矩阵来计算自适应权矢量,虽然在期望信号功率较强时具有较好的性能,但是该方法在实际应用中存在如下两个问题:第一,该方法要求阵列构型是精确已知的,唯一允许的误差是观测角误差,在考虑互偶效应时性能大幅度下降;第二,该方法在重构干扰加噪声协方差矩阵时计算复杂度很大,使得算法的实时性受到制约。In 1991, Benjamin Friedlander and W Anthony J. Weiss proposed a DOA estimation method when there is mutual coupling between array elements, which can accurately estimate the DOA of the signal's direction of arrival and the mutual coupling between uniform circular arrays, but The DOA estimation method in the presence of mutual coupling between array elements has not been applied in the field of adaptive beamforming technology; in 2012, Gu proposed a beamforming method based on the reconstruction of the interference plus noise covariance matrix. The constructed covariance matrix replaces the expected polluted sampling covariance matrix to calculate the adaptive weight vector. Although it has better performance when the expected signal power is stronger, this method has the following two problems in practical applications: first , this method requires that the array configuration is known precisely, and the only allowable error is the observation angle error, and the performance is greatly degraded when considering the mutual coupling effect; second, the method is computationally complex when reconstructing the interference-plus-noise covariance matrix The degree is very large, which restricts the real-time performance of the algorithm.

发明内容Contents of the invention

针对上述现有技术的不足,本发明的目的在于提出一种基于迭代互耦校正的雷达协方差矩阵重构波束形成方法,该种基于迭代互耦校正的雷达协方差矩阵重构波束形成方法对信号的入射角度和均匀圆阵的互耦矩阵进行迭代估计,结合干扰加噪声协方差矩阵重构方法,完成干扰加噪声协方差矩阵的重构和期望导向矢量的修正,得到一种在阵元存在互耦的条件下更加稳健的波束形成器。In view of the deficiencies in the prior art above, the purpose of the present invention is to propose a radar covariance matrix reconstruction beamforming method based on iterative mutual coupling correction, which is based on the iterative mutual coupling correction radar covariance matrix reconstruction beamforming method The incident angle of the signal and the mutual coupling matrix of the uniform circular array are iteratively estimated, combined with the reconstruction method of the interference plus noise covariance matrix, the reconstruction of the interference plus noise covariance matrix and the correction of the desired steering vector are completed, and an array element A more robust beamformer in the presence of mutual coupling.

为达到上述目的,本发明采用如下技术方案予以实现。In order to achieve the above object, the present invention adopts the following technical solutions to achieve.

一种基于迭代互耦校正的雷达协方差矩阵重构波束形成方法,包括以下步骤:A radar covariance matrix reconstruction beamforming method based on iterative mutual coupling correction, comprising the following steps:

步骤1,确定均匀圆阵,该均匀圆阵包括M个阵元,均匀圆阵设定范围内存在Q个信号源,Q个信号源向均匀圆阵发射Q个入射信号,所述Q个入射信号包含1个期望信号和Q-1个干扰信号;Step 1, determine the uniform circular array, the uniform circular array includes M array elements, there are Q signal sources within the set range of the uniform circular array, and the Q signal sources transmit Q incident signals to the uniform circular array, and the Q incident signals The signal contains 1 desired signal and Q-1 interference signals;

获取均匀圆阵的采样协方差矩阵R,并对所述均匀圆阵的采样协方差矩阵R进行特征分解,得到M个特征值;M、Q分别为大于0的正整数,Q>1,M表示均匀圆阵包括的阵元个数,与对均匀圆阵的采样协方差矩阵R进行特征分解后得到的特征值个数取值相等;Obtain the sampling covariance matrix R of the uniform circular array, and perform eigendecomposition on the sampling covariance matrix R of the uniform circular array to obtain M eigenvalues; M and Q are respectively positive integers greater than 0, Q>1, M Indicates the number of array elements included in the uniform circular array, which is equal to the number of eigenvalues obtained after eigendecomposing the sampling covariance matrix R of the uniform circular array;

步骤2,计算入射方向为(θ,φ)的信号MUSIC谱,然后设定均匀圆阵的互耦矩阵初始值,进而得到Q个入射信号的Q个方位角初始值,分别为q∈{0,1,2,…,Q-1},表示第q+1个入射信号的方位角初始值;Step 2, calculate the MUSIC spectrum of the signal with the incident direction (θ, φ), and then set the initial value of the mutual coupling matrix of the uniform circular array, and then obtain the initial values of Q azimuth angles of the Q incident signals, respectively q ∈ {0,1,2,...,Q-1}, Indicates the initial value of the azimuth angle of the q+1th incident signal;

初始化:令k表示第k次修正,k的初始值为1;令第k次修正后均匀圆阵的互耦矩阵为Ck,并将Q个入射信号的Q个方位角初始值作为第0次修正后Q个入射信号的方位角θ0;设定均匀圆阵的互耦矩阵初始值为C0,C0=IM,IM表示M×M维单位矩阵;Initialization: let k represent the kth correction, and the initial value of k is 1; let the mutual coupling matrix of the uniform circular array after the kth correction be C k , and set the initial values of Q azimuth angles of the Q incident signals as the 0th The azimuth angle θ 0 of the Q incident signals after the second correction; the initial value of the mutual coupling matrix of the uniform circular array is set to C 0 , C 0 =I M , and I M represents the M×M dimensional identity matrix;

步骤3,根据第k次修正后均匀圆阵的互耦矩阵Ck对Q个入射信号分别进行波达方向估计,得到第k次修正后入射方向为(θk,φ)的信号MUSIC谱PMUSICk,φ),以及第k次修正后Q个入射信号的方位角;Step 3: According to the mutual coupling matrix C k of the uniform circular array after the k-th correction, the direction of arrival is estimated for the Q incident signals respectively, and the MUSIC spectrum P of the signal whose incident direction is (θ k , φ) after the k-th correction is obtained MUSICk ,φ), and the azimuth angles of the Q incident signals after the kth correction;

步骤4,依次得到第k次修正后Q个入射信号的MUSIC谱值倒数的和Jck的定义式和计算式,进而计算得到第k次修正后均匀圆阵的互耦矩阵CkStep 4, sequentially obtain the definition formula and calculation formula of the reciprocal sum J ck of the MUSIC spectrum values of the Q incident signals after the k-th correction, and then calculate the mutual coupling matrix C k of the uniform circular array after the k-th correction;

步骤5,令k加1,返回步骤3,直到Jck-Jc(k-1)<△,则修正迭代结束,Jc(k-1)表示第k-1次修正后Q个入射信号的MUSIC谱值倒数的和,△表示设定的门限值,并分别将修正迭代停止时对应的第k次修正后均匀圆阵的互耦矩阵Ck,记为均匀圆阵的最终互偶矩阵将修正迭代停止时对应的第k次修正后Q个入射信号的方位角,记为Q个入射信号的最终方位角 Step 5, increase k by 1, return to step 3, until J ck -J c(k-1) <△, then the correction iteration ends, J c(k-1) represents the Q incident signals after the k-1th correction The sum of the reciprocals of the MUSIC spectrum values of , △ represents the set threshold value, and the mutual coupling matrix C k of the uniform circular array corresponding to the kth correction when the correction iteration stops is recorded as the final mutual coupling matrix of the uniform circular array matrix The azimuth angles of the Q incident signals corresponding to the kth correction when the correction iteration stops are recorded as the final azimuth angles of the Q incident signals

步骤6,根据均匀圆阵的最终互偶矩阵和Q个入射信号的最终方位角计算得到重构后均匀圆阵的干扰加噪声协方差矩阵 Step 6, according to the final mutual dual matrix of the uniform circular array and the final azimuths of the Q incident signals Calculate the interference plus noise covariance matrix of the reconstructed uniform circular array

步骤7,计算得到期望信号的最终导向矢量为并根据重构后均匀圆阵的干扰加噪声协方差矩阵计算得到均匀圆阵的自适应波束形成器的权矢量为w,进而完成了基于迭代互耦校正的均匀圆阵干扰加噪声协方差矩阵重构的波束形成设计。Step 7, calculate the final steering vector of the desired signal as And according to the interference plus noise covariance matrix of the uniform circular array after reconstruction The weight vector of the adaptive beamformer of the uniform circular array is calculated as w, and then the beamforming design of the uniform circular array interference plus noise covariance matrix reconstruction based on iterative mutual coupling correction is completed.

本发明的有益效果:第一,本发明使用DOA与均匀圆阵互耦矩阵迭代估计的方法较为准确的估计出在互耦影响下的干扰加噪声协方差矩阵重构中不可或缺的两个参量,即均匀圆阵的互耦矩阵和干扰信号的方位角,使得干扰加噪声协方差矩阵的重构充分携带了互耦信息,提升了在互耦影响下的波束形成器的稳健性;第二,本发明采用在干扰角度区域取离散点而非积分的方法来重构干扰协方差矩阵,降低了计算复杂度,提高了算法的实时性。Beneficial effects of the present invention: First, the present invention uses the DOA and uniform circular array mutual coupling matrix iterative estimation method to more accurately estimate the two indispensable factors in the reconstruction of the interference plus noise covariance matrix under the influence of mutual coupling The parameters, that is, the mutual coupling matrix of the uniform circular array and the azimuth angle of the interference signal, make the reconstruction of the interference plus noise covariance matrix fully carry the mutual coupling information, and improve the robustness of the beamformer under the influence of mutual coupling; Second, the present invention reconstructs the interference covariance matrix by taking discrete points instead of integrals in the interference angle area, which reduces the computational complexity and improves the real-time performance of the algorithm.

附图说明Description of drawings

为了更清楚地说明本发明实施例或现有技术中的技术方案,下面将对实施例或现有技术描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to more clearly illustrate the technical solutions in the embodiments of the present invention or the prior art, the following will briefly introduce the drawings that need to be used in the description of the embodiments or the prior art. Obviously, the accompanying drawings in the following description are only These are some embodiments of the present invention. Those skilled in the art can also obtain other drawings based on these drawings without creative work.

图1为本发明的一种基于迭代互耦校正的雷达协方差矩阵重构波束形成方法流程图;Fig. 1 is a flow chart of a radar covariance matrix reconstruction beamforming method based on iterative mutual coupling correction of the present invention;

图2为互耦条件下存在观测误差时本发明方法性能随信噪比(SNR)变化曲线图;Fig. 2 is that the method performance of the present invention varies with the signal-to-noise ratio (SNR) when there is an observation error under the mutual coupling condition;

图3(a)为互耦条件下存在观测误差且输入信噪比为20dB时本发明方法性能随样本数变化曲线图;Fig. 3 (a) is that there is observation error under the condition of mutual coupling and the input SNR is 20dB when the method performance of the present invention changes with sample number;

图3(b)为互耦条件下存在观测误差且输入信噪比为-5dB时本发明方法性能随样本数变化曲线图;Fig. 3 (b) is that there is observation error under the condition of mutual coupling and input signal-to-noise ratio is -5dB when the method performance of the present invention changes with sample number;

图4为互耦条件下无观测误差时本发明方法性能随SNR变化曲线图;Fig. 4 is when there is no observation error under the condition of mutual coupling, the method performance of the present invention changes curve figure with SNR;

图5(a)为互耦条件下无观测误差且输入信噪比为20dB时本发明方法性能随样本数变化曲线图;Fig. 5 (a) is no observation error under the condition of mutual coupling and the input signal-to-noise ratio is 20dB when the method performance of the present invention changes with sample number curve;

图5(b)为互耦条件下无观测误差且输入信噪比为-5dB时本发明方法性能随样本数变化曲线图。Fig. 5(b) is a graph showing the variation of the performance of the method of the present invention with the number of samples when there is no observation error and the input signal-to-noise ratio is -5dB under mutual coupling conditions.

具体实施方式Detailed ways

下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。The following will clearly and completely describe the technical solutions in the embodiments of the present invention with reference to the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only some, not all, embodiments of the present invention. Based on the embodiments of the present invention, all other embodiments obtained by persons of ordinary skill in the art without making creative efforts belong to the protection scope of the present invention.

参照图1,为本发明的一种基于迭代互耦校正的雷达协方差矩阵重构波束形成方法流程图;其中所述基于迭代互耦校正的雷达协方差矩阵重构波束形成方法,包括以下步骤:Referring to Fig. 1, it is a flow chart of a radar covariance matrix reconstruction beamforming method based on iterative mutual coupling correction of the present invention; wherein the radar covariance matrix reconstruction beamforming method based on iterative mutual coupling correction comprises the following steps :

步骤1,确定均匀圆阵,该均匀圆阵包括M个阵元,获取均匀圆阵的采样协方差矩阵R,对所述均匀圆阵的采样协方差矩阵R进行特征分解,得到M个特征值;其中M为大于0的正整数。Step 1, determine the uniform circular array, the uniform circular array includes M array elements, obtain the sampling covariance matrix R of the uniform circular array, perform eigendecomposition on the sampling covariance matrix R of the uniform circular array, and obtain M eigenvalues ; Where M is a positive integer greater than 0.

具体地,确定均匀圆阵,该均匀圆阵包括M个阵元,均匀圆阵设定范围内存在Q个信号源,Q个信号源向均匀圆阵发射Q个入射信号,所述Q个入射信号包含1个期望信号和Q-1个干扰信号;所述设定范围内为距离均匀圆阵S千米以内,S为大于0的正整数;本实施例中S取值为100。Specifically, a uniform circular array is determined, the uniform circular array includes M array elements, there are Q signal sources within the set range of the uniform circular array, and the Q signal sources transmit Q incident signals to the uniform circular array, and the Q incident signals The signal includes 1 desired signal and Q-1 interference signals; the set range is within S kilometers from the uniform circular array, and S is a positive integer greater than 0; the value of S is 100 in this embodiment.

Q个入射信号相对于均匀圆阵的俯仰角为φ,φ={φ01,…,φq,…,φQ-1},q∈{0,1,…,Q-1},φq表示第q+1个入射信号相对于均匀圆阵的俯仰角,且φ0、φ1、…、φq、…、φQ-1取值分别相等;φ0表示期望信号相对于均匀圆阵的俯仰角,Q-1个干扰信号相对于均匀圆阵的俯仰角分别为φ1、φ2、…、φQ-1The pitch angle of the Q incident signals relative to the uniform circular array is φ, φ={φ 01 ,…,φ q ,…,φ Q-1 }, q∈{0,1,…,Q-1} , φ q represents the pitch angle of the q+1th incident signal relative to the uniform circular array, and the values of φ 0 , φ 1 , ..., φ q , ..., φ Q-1 are equal; φ 0 represents the desired signal relative to The pitch angles of the uniform circular array, the pitch angles of the Q-1 interference signals relative to the uniform circular array are φ 1 , φ 2 , ..., φ Q-1 respectively.

获取均匀圆阵接收到的回波数据,并对所述均匀圆阵接收到的回波数据进行自相关处理,得到均匀圆阵的采样协方差矩阵R。The echo data received by the uniform circular array is acquired, and autocorrelation processing is performed on the echo data received by the uniform circular array to obtain a sampling covariance matrix R of the uniform circular array.

在已知期望信号个数为1、干扰信号个数为Q-1,以及Q个入射信号相对于均匀圆阵的俯仰角为φ的前提下,对均匀圆阵的采样协方差矩阵R进行特征分解,得到M个特征值;由于均匀圆阵的阵元个数为M,则经过特征分解后得到的特征值个数也为M。Under the premise that the number of expected signals is 1, the number of interference signals is Q-1, and the pitch angle of Q incident signals relative to the uniform circular array is φ, the sampling covariance matrix R of the uniform circular array is characterized Decompose to obtain M eigenvalues; since the number of array elements of the uniform circular array is M, the number of eigenvalues obtained after eigendecomposition is also M.

对特征分解后得到的M个特征值进行从大到小排序,并分别将从大到小排序后的M个特征值中前Q个特征值记为Q个大特征值,将其余M-Q个特征值记为M-Q个小特征值;将前Q个大特征值对应的特征向量,作为期望信号加干扰子空间,将M-Q个小特征值对应的特征向量,记为噪声子空间,则对均匀圆阵的采样协方差矩阵R进行特征分解,其分解形式为:The M eigenvalues obtained after eigendecomposition are sorted from large to small, and the first Q eigenvalues of the M eigenvalues sorted from large to small are recorded as Q large eigenvalues, and the remaining M-Q eigenvalues are The value is recorded as M-Q small eigenvalues; the eigenvectors corresponding to the first Q large eigenvalues are used as the desired signal plus interference subspace, and the eigenvectors corresponding to M-Q small eigenvalues are recorded as the noise subspace, then for the uniform circle The sampling covariance matrix R of the array is subjected to eigendecomposition, and its decomposition form is:

其中,R为均匀圆阵的采样协方差矩阵,维数为M×M;ΛSI为Q个大特征值分别为对角元素形成的对角矩阵,USI为Q个大特征值对应的特征向量形成的期望信号加干扰子空间,ΛN为M-Q个小特征值分别为对角元素形成的对角矩阵,UN为M-Q个小特征值对应的特征向量形成的噪声子空间,上标H表示共轭转置操作,M、Q分别为大于0的正整数,M>Q;M表示均匀圆阵包括的阵元个数,与对均匀圆阵的采样协方差矩阵R进行特征分解后得到的特征值个数取值相等。Among them, R is the sampling covariance matrix of the uniform circular array, and its dimension is M×M; Λ SI is a diagonal matrix formed by the Q large eigenvalues respectively being diagonal elements, and U SI is the characteristic corresponding to the Q large eigenvalues The desired signal plus interference subspace formed by the vector, Λ N is a diagonal matrix formed by MQ small eigenvalues respectively as diagonal elements, U N is the noise subspace formed by the eigenvectors corresponding to MQ small eigenvalues, superscript H Represents the conjugate transpose operation, M and Q are positive integers greater than 0, M>Q; M represents the number of array elements included in the uniform circular array, which is obtained after eigendecomposition of the sampling covariance matrix R of the uniform circular array The number of eigenvalues of is equal.

步骤2,计算入射方向为(θ,φ)的信号MUSIC谱,然后设定均匀圆阵的互耦矩阵初始值,则入射方向为(θ,φ)的信号MUSIC谱就有了一个初始估计值;将均匀圆阵的互耦矩阵初始值代入入射方向为(θ,φ)的信号MUSIC谱PMUSIC(θ,φ)表达式中,并在设定方位角范围内搜索MUSIC谱峰,进而得到Q个入射信号的Q个方位角初始值,分别为 Step 2, calculate the MUSIC spectrum of the signal with the incident direction (θ, φ), and then set the initial value of the mutual coupling matrix of the uniform circular array, then the MUSIC spectrum of the signal with the incident direction (θ, φ) has an initial estimated value ; Substitute the initial value of the mutual coupling matrix of the uniform circular array into the expression of the signal MUSIC spectrum P MUSIC (θ, φ) with the incident direction (θ, φ), and search for the MUSIC spectrum peak within the set azimuth angle range, and then get The initial values of Q azimuth angles for the Q incident signals are respectively

具体地,所述入射方向为(θ,φ)的信号MUSIC谱PMUSIC(θ,φ),其表达式为:Specifically, the signal MUSIC spectrum P MUSIC (θ, φ) whose incident direction is (θ, φ) is expressed as:

其中,θ表示Q个入射信号的方位角,φ表示Q个入射信号相对于均匀圆阵的俯仰角,a(θ,φ)为入射方向为(θ,φ)的信号导向矢量,C为均匀圆阵的互耦矩阵,且均匀圆阵的互耦矩阵C是未知的;UN为M-Q个小特征值对应的特征向量形成的噪声子空间,上标H表示共轭转置操作。Among them, θ represents the azimuth angle of the Q incident signals, φ represents the elevation angle of the Q incident signals relative to the uniform circular array, a(θ, φ) is the signal steering vector with the incident direction (θ, φ), and C is the uniform The mutual coupling matrix of the circular array, and the mutual coupling matrix C of the uniform circular array is unknown; U N is the noise subspace formed by the eigenvectors corresponding to MQ small eigenvalues, and the superscript H represents the conjugate transpose operation.

设定均匀圆阵的互耦矩阵初始值C0,C0=IM,IM表示M×M维单位矩阵;将均匀圆阵的互耦矩阵初始值C0代入入射方向为(θ,φ)的信号MUSIC谱PMUSIC(θ,φ)表达式中,并在0°到180°方位角范围内搜索MUSIC谱峰,进而得到Q个入射信号的Q个方位角初始值,分别为表示第q+1个入射信号的方位角初始值;其中,设定方位角范围内为0°到180°范围内。Set the initial value C 0 of the mutual coupling matrix of the uniform circular array, C 0 =I M , I M represents the M×M dimensional unit matrix; substitute the initial value C 0 of the mutual coupling matrix of the uniform circular array into the incident direction as (θ,φ ) signal MUSIC spectrum P MUSIC (θ, φ) expression, and search the MUSIC spectrum peak in the range of 0° to 180° azimuth angle, and then get the initial values of Q azimuth angles of Q incident signals, respectively Indicates the initial value of the azimuth angle of the q+1th incident signal; wherein, the range of the set azimuth angle is within the range of 0° to 180°.

初始化:令k表示第k次修正,k的初始值为1;并将Q个入射信号的Q个方位角初始值作为第0次修正后Q个入射信号的方位角θ0;设定均匀圆阵的互耦矩阵初始值为C0,C0=IM,IM表示M×M维单位矩阵。Initialization: Let k represent the kth correction, and the initial value of k is 1; and the initial value of the Q azimuth angles of the Q incident signals is taken as the azimuth angle θ 0 of the Q incident signals after the 0th correction; set the uniform circle The initial value of the mutual coupling matrix of the array is C 0 , C 0 =I M , and I M represents the M×M dimensional identity matrix.

步骤3,特征分解完成后,在考虑均匀圆阵互耦的情况下,令第k次修正后均匀圆阵的互耦矩阵为Ck,并根据第k次修正后均匀圆阵的互耦矩阵Ck使用MUSIC谱估计方法对Q个入射信号分别进行波达方向(DOA)估计,得到第k次修正后入射方向为(θk,φ)的信号MUSIC谱PMUSICk,φ)。Step 3, after the eigendecomposition is completed, in the case of considering the mutual coupling of the uniform circular array, let the mutual coupling matrix of the uniform circular array after the k-th correction be C k , and according to the mutual coupling matrix of the uniform circular array after the k-th correction C k uses the MUSIC spectrum estimation method to estimate the direction of arrival (DOA) of the Q incident signals respectively, and obtain the signal MUSIC spectrum P MUSICk , φ) with the incident direction (θ k , φ) after the kth correction.

具体地,在考虑均匀圆阵互耦的情况下,根据第k次修正后均匀圆阵的互耦矩阵Ck使用MUSIC谱估计方法对入射的期望信号和Q-1个干扰信号进行波达方向(DOA)估计,计算得到第k次修正后入射方向为(θk,φ)的信号MUSIC谱PMUSICk,φ),其表达式为:Specifically, in the case of considering the mutual coupling of the uniform circular array, according to the mutual coupling matrix C k of the uniform circular array after the kth correction, the MUSIC spectrum estimation method is used to calculate the direction of arrival (DOA) of the incident desired signal and Q-1 interference signals (DOA) estimation, calculate the signal MUSIC spectrum P MUSICk ,φ) with the incident direction (θ k ,φ) after the kth correction, and its expression is:

其中,θk表示第k次修正后Q个入射信号的方位角,φ表示Q个入射信号相对于均匀圆阵的俯仰角,a(θk,φ)为入射方向为(θk,φ)的信号导向矢量,Ck为第k次修正后均匀圆阵的互耦矩阵,且第k次修正后均匀圆阵的互耦矩阵是未知的;UN为M-Q个小特征值对应的特征向量形成的噪声子空间,上标H表示共轭转置操作。Among them, θ k represents the azimuth angle of the Q incident signals after the kth correction, φ represents the elevation angle of the Q incident signals relative to the uniform circular array, and a(θ k , φ) is the incident direction as (θ k , φ) , C k is the mutual coupling matrix of the uniform circular array after the k-th correction, and the mutual coupling matrix of the uniform circular array after the k-th correction is unknown; U N is the eigenvector corresponding to the MQ small eigenvalues The noise subspace formed, the superscript H indicates the conjugate transpose operation.

由于第k次修正后均匀圆阵的互耦矩阵C是未知的,入射方向为(θk,φ)的信号MUSIC谱PMUSICk,φ)无法计算,那么期望信号和干扰信号的波达方向(DOA)就是未知的。Since the mutual coupling matrix C of the uniform circular array after the k-th correction is unknown, the signal MUSIC spectrum P MUSICk ,φ) with the incident direction (θ k ,φ) cannot be calculated, then the waves of the desired signal and the interference signal The direction of arrival (DOA) is unknown.

在设定方位角范围内搜索第k次修正后入射方向为(θk,φ)的信号MUSIC谱PMUSICk,φ)的MUSIC谱峰,得到第k次修正后Q个入射信号的方位角为θk,θk={θ0k1k,…,θqk,…,θ(Q-1)k},q∈{0,1,…,Q-1},θqk表示第k次修正后第q+1个入射信号的方位角;θ0k表示第k次修正后期望信号的方位角,θ1k2k,…,θ(Q-1)k为第k次修正后Q-1个干扰信号的方位角;其中,设定方位角范围内为0°到180°范围内。Search for the MUSIC spectrum peak of the signal MUSIC spectrum P MUSICk , φ) with the incident direction (θ k , φ) after the k-th correction within the range of the set azimuth angle, and obtain the MUSIC spectrum peak of the Q incident signal after the k-th correction The azimuth angle is θ k , θ k ={θ 0k1k ,…,θ qk ,…,θ (Q-1)k }, q∈{0,1,…,Q-1}, θ qk represents the The azimuth angle of the q+1th incident signal after the k-th correction; θ 0k represents the azimuth angle of the expected signal after the k-th correction, θ 1k , θ 2k ,…, θ (Q-1)k is the k-th correction The azimuth angles of Q-1 interference signals; wherein, the set azimuth angles range from 0° to 180°.

步骤4,定义第k次修正后Q个入射信号的MUSIC谱值倒数的和为Jck,由步骤3可知,当第k次修正后均匀圆阵的互耦矩阵与实际的均匀圆阵的互耦矩阵取值相等,则第k次修正后Q个入射信号的MUSIC谱值倒数的和Jck具有最小值;如果第k次修正后均匀圆阵的互耦矩阵与实际的均匀圆阵的互耦矩阵取值不相等,则第k次修正后Q个入射信号的MUSIC谱值倒数的和Jck没有最小值;那么在已经得到第k次修正后Q个入射信号的Q个方位角情况下,让第k次修正后Q个入射信号的MUSIC谱值倒数的和Jck取值最小,进而计算得到第k次修正后均匀圆阵的互耦矩阵CkStep 4, define the sum of the reciprocals of the MUSIC spectrum values of the Q incident signals after the k-th correction as J ck , from step 3, when the mutual coupling matrix of the uniform circular array after the k-th correction and the actual uniform circular array If the values of the coupling matrices are equal, the sum J ck of the reciprocals of the MUSIC spectrum values of the Q incident signals after the k-th correction has the minimum value; if the mutual coupling matrix of the uniform circular array and the actual uniform circular array after the k-th correction If the values of the coupling matrices are not equal, the sum J ck of the reciprocals of the MUSIC spectrum values of the Q incident signals after the kth correction has no minimum value; then, if the Q azimuths of the Q incident signals after the kth correction have been , let the sum J ck of the reciprocals of the MUSIC spectrum values of the Q incident signals after the k-th correction be the smallest, and then calculate the mutual coupling matrix C k of the uniform circular array after the k-th correction.

步骤4具体包括如下子步骤:Step 4 specifically includes the following sub-steps:

(4a)根据第k次修正后均匀圆阵的互耦矩阵Ck,定义第k次修正后Q个入射信号的MUSIC谱值倒数的和为Jck,其定义表达式为:(4a) According to the mutual coupling matrix C k of the uniform circular array after the k-th correction, the sum of the reciprocals of the MUSIC spectrum values of the Q incident signals after the k-th correction is defined as J ck , and the definition expression is:

其中,表示入射方向为的信号导向矢量,φq表示第q+1个入射信号相对于均匀圆阵的俯仰角,表示第k次修正后第q+1个入射信号的方位角,||||2表示取模值之后再求平方操作;Ck为第k次修正后均匀圆阵的互耦矩阵,UN为M-Q个小特征值对应的特征向量形成的噪声子空间,上标H表示共轭转置操作。in, Indicates that the direction of incidence is The signal steering vector of , φ q represents the pitch angle of the q+1th incident signal relative to the uniform circular array, Indicates the azimuth angle of the q+1th incident signal after the kth correction, |||| 2 represents the square operation after taking the modulus value; C k is the mutual coupling matrix of the uniform circular array after the kth correction, U N is the noise subspace formed by the eigenvectors corresponding to MQ small eigenvalues, and the superscript H represents the conjugate transpose operation.

则由步骤3可知,当设定的均匀圆阵的互耦矩阵初始估计值与实际的均匀圆阵的互耦矩阵取值不相等,则第k次修正后Q个入射信号的MUSIC谱值倒数的和Jck没有最小值;那么在已经得到第k次修正后Q个入射信号的Q个方位角估计值的情况下,让第k次修正后Q个入射信号的MUSIC谱值倒数的和取值最小,来修正均匀圆阵的互耦矩阵,即求解第k次修正后Q个入射信号的MUSIC谱值倒数的和Jck取值最小时对应的第k次修正后均匀圆阵的互耦矩阵。It can be seen from step 3 that when the initial estimated value of the mutual coupling matrix of the uniform circular array is not equal to the value of the actual mutual coupling matrix of the uniform circular array, the reciprocal of the MUSIC spectrum values of the Q incident signals after the kth correction The sum of J ck has no minimum value; then, in the case that Q azimuth angle estimates of the Q incident signals after the k-th correction have been obtained, let the sum of the reciprocals of the MUSIC spectrum values of the Q incident signals after the k-th correction be taken as The value is the smallest, to modify the mutual coupling matrix of the uniform circular array, that is, to solve the mutual coupling of the uniform circular array after the kth correction corresponding to the reciprocal of the MUSIC spectrum values of the Q incident signals after the kth correction and the value of J ck is the smallest matrix.

(4b)由于均匀圆阵的互耦矩阵具有一些特殊的性质:第一,均匀圆阵的互耦矩阵是一个对称矩阵;第二,均匀圆阵相邻两阵元相距的距离越大,彼此之间的互阻抗就越小;第三,均匀圆阵闭合的几何结构,即编号为2的阵元对编号为1的阵元的互阻抗,与编号为1的阵元对编号为2的阵元的互阻抗取值相等。(4b) Because the mutual coupling matrix of the uniform circular array has some special properties: first, the mutual coupling matrix of the uniform circular array is a symmetrical matrix; second, the greater the distance between two adjacent array elements of the uniform circular array, the greater the mutual The smaller the mutual impedance between; third, the closed geometric structure of the uniform circular array, that is, the mutual impedance of the array element numbered 2 to the array element numbered 1, and the array element numbered 1 to the array element numbered 2 The mutual impedance values of the array elements are equal.

基于以上特性,第k次修正后均匀圆阵的互耦矩阵Ck是一个复循环对称矩阵,可以由第k次修正后均匀圆阵的互耦矩阵Ck第一行中的前LC个元素完全确定,表示向下取整操作;并且确定第k次修正后均匀圆阵的互耦矩阵Ck与入射方向为(θk,φ)的信号导向矢量a(θk,φ)的乘积,等价于入射方向为(θk,φ)的信号导向矢量a(θk,φ)中的M个元素组成的M×LC维矩阵Q[a(θk,φ)]与第k次修正后均匀圆阵的互耦矩阵Ck中第一行的前LC个元素完组成的LC×1维向量ck的乘积,即Cka(θk,φ)=Q[a(θk,φ)]ckBased on the above characteristics, the mutual coupling matrix C k of the uniform circular array after the k-th correction is a complex circular symmetric matrix, which can be obtained from the first LC in the first row of the mutual coupling matrix C k of the uniform circular array after the k-th correction elements are fully identified, Represents the rounding down operation; and determine the product of the mutual coupling matrix C k of the uniform circular array after the kth correction and the signal steering vector a(θ k , φ) with the incident direction (θ k , φ), which is equivalent to The M×L C -dimensional matrix Q[a(θ k ,φ)] composed of M elements in the signal steering vector a(θ k ,φ) with the incident direction (θ k ,φ) is equal to The product of LC × 1-dimensional vector c k formed by the first LC elements of the first row in the mutual coupling matrix C k of the circular array, that is, C k a(θ k ,φ)=Q[a(θ k , φ)] c k .

其中,ck为第k次修正后均匀圆阵的互耦矩阵Ck中第一行的前LC个元素组成的LC×1维向量,cdk表示第k次修正后均匀圆阵的互耦矩阵Ck中第一行的第d+1个元素,上标T表示转置操作。Among them, c k is the LC × 1-dimensional vector composed of the first LC elements in the first row of the mutual coupling matrix C k of the uniform circular array after the k-th correction, c dk represents the d+1th element in the first row of the mutual coupling matrix C k of the uniform circular array after the kth correction, and the superscript T represents the transpose operation.

入射方向为(θk,φ)的信号导向矢量a(θk,φ)中的M个元素组成的M×LC维矩阵Q[a(θk,φ)]由第k次修正后的第一M×LC维矩阵Q1k、第k次修正后的第二M×LC维矩阵Q2k、第k次修正后的第三M×LC维矩阵Q3k和第k次修正后的第四M×LC维矩阵Q4k相加得到,即Q[a(θk,φ)]=Q1k+Q2k+Q3k+Q4k,第k次修正后的第一M×LC维矩阵Q1k、第k次修正后的第二M×LC维矩阵Q2k、第k次修正后的第三M×LC维矩阵Q3k和第k次修正后的第四M×LC维矩阵Q4k分别由入射方向为(θk,φ)的信号导向矢量a(θk,φ)中的元素构成,其中第k次修正后的第一M×LC维矩阵Q1k中第r行、第h列元素为Q1(r,h)k,第k次修正后的第二M×LC维矩阵Q2k中第r'行、第h'列元素为Q2(r',h')k,第k次修正后的第三M×LC维矩阵Q3中第r”行、第h”列元素为Q3(r”,h”)k,第k次修正后的第四M×LC维矩阵Q4中第r”'行、第h”'列元素为Q4(r”',h”')k,表达式分别为:The M×L C -dimensional matrix Q[a(θ k ,φ)] composed of M elements in the signal steering vector a(θ k ,φ) with the incident direction (θ k ,φ) is modified by the kth The first M×L C -dimensional matrix Q 1k , the second M×L C -dimensional matrix Q 2k after the k-th correction, the third M×L C -dimensional matrix Q 3k after the k-th correction, and the k-th correction The fourth M×L C -dimensional matrix Q 4k is obtained by adding, that is, Q[a(θ k ,φ)]=Q 1k +Q 2k +Q 3k +Q 4k , the first M×L after the kth correction C -dimensional matrix Q 1k , the second M×L C -dimensional matrix Q 2k after the k-th correction, the third M×L C -dimensional matrix Q 3k after the k-th correction, and the fourth M×L C-dimensional matrix Q 3k after the k-th correction The L C -dimensional matrix Q 4k is composed of the elements in the signal-steering vector a(θ k , φ) with the incident direction (θ k , φ), where the first M×L C -dimensional matrix Q 1k after the kth correction The element in row r and column h in is Q 1(r,h)k , and the element in row r' and column h' in the second M×L C -dimensional matrix Q 2k after the kth correction is Q 2( r',h')k , the third M×L C -dimensional matrix Q 3 after the k-th correction, the elements in the r"th row and the h"th column are Q 3(r",h")k , the k-th The element in row r"' and column h"' in the fourth M×L C -dimensional matrix Q 4 after modification is Q 4(r"',h"')k , and the expressions are respectively:

其中,r∈{1,2,…,row1k},h∈{1,2,…,col1k},row1k表示第k次修正后的第一M×LC维矩阵Q1k的行数,col1k表示第k次修正后的第一M×LC维矩阵Q1k的列数,r'∈{1,2,…,row2k},h'∈{1,2,…,col2k},row2k表示第k次修正后的第二M×LC维矩阵Q2k的行数,col2k表示第k次修正后的第二M×LC维矩阵Q2k的列数,r”∈{1,2,…,row3k},h”∈{1,2,…,col3k},row3k表示第k次修正后的第三M×LC维矩阵Q3k的行数,col3k表示第k次修正后的第三M×LC维矩阵Q3k的列数,r”'∈{1,2,…,row4k},h”'∈{1,2,…,col4k},row4k表示第k次修正后的第四M×LC维矩阵Q4k的行数,col4k表示第k次修正后的第四M×LC维矩阵Q4k的列数,表示向上取整操作;a(θk,φ)r+h-1表示入射方向为(θk,φ)的信号导向矢量a(θk,φ)中第r+h-1个元素,a(θk,φ)r'-h'+1表示入射方向为(θk,φ)的信号导向矢量a(θk,φ)中第r'-h'+1个元素,a(θk,φ)M+1+r”-h”表示入射方向为(θk,φ)的信号导向矢量a(θk,φ)中第M+1+r”-h”个元素,a(θk,φ)r”'+h”'-M-1表示入射方向为(θk,φ)的信号导向矢量a(θk,φ)中第r”'+h”'-M-1个元素;θk表示第k次修正后Q个入射信号的方位角,且第0次修正后Q个入射信号的方位角θ0为Q个入射信号的Q个方位角初始值。Among them, r∈{1,2,…,row 1k }, h∈{1,2,…,col 1k }, row 1k represents the number of rows of the first M×L C -dimensional matrix Q 1k after the kth correction , col 1k represents the number of columns of the first M×L C -dimensional matrix Q 1k after the kth correction, r'∈{1,2,...,row 2k }, h'∈{1,2,...,col 2k }, row 2k represents the row number of the second M×L C -dimensional matrix Q 2k after the k-th correction, col 2k represents the column number of the second M×L C -dimensional matrix Q 2k after the k-th correction, r” ∈{1,2,…,row 3k }, h”∈{1,2,…,col 3k }, row 3k represents the number of rows of the third M×L C -dimensional matrix Q 3k after the kth correction, col 3k represents the number of columns of the third M×L C -dimensional matrix Q 3k after the kth correction, r"'∈{1,2,...,row 4k }, h"'∈{1,2,...,col 4k }, row 4k represents the number of rows of the fourth M×L C -dimensional matrix Q 4k after the k correction, and col 4k represents the column number of the fourth M×L C -dimensional matrix Q 4k after the k correction, Represents an upward rounding operation; a(θ k ,φ) r+h-1 represents the r+h-1th element in the signal steering vector a(θ k ,φ) with the incident direction (θ k ,φ), a (θ k ,φ) r'-h'+1 represents the r'-h'+1th element in the signal steering vector a(θ k ,φ) with the incident direction (θ k ,φ), a(θ k ,φ) M+1+r”-h” represents the M+1+r”-h”th element in the signal steering vector a(θ k ,φ) with the incident direction (θ k ,φ), a(θ k , φ) r"'+h"'-M-1 means the r"'+h"'-M-1 of the signal steering vector a(θ k ,φ) with the incident direction (θ k ,φ) Elements; θ k represents the azimuth angles of the Q incident signals after the kth correction, and the azimuth angle θ 0 of the Q incident signals after the 0th correction is the initial value of the Q azimuth angles of the Q incident signals.

(4c)由(4b)所描述的均匀圆阵的互耦矩阵性质可以得到,第k次修正后的均匀圆阵的互耦矩阵Ck与入射方向为的信号导向矢量可以进行等价代换,即其中,ck为第k次修正后均匀圆阵的互耦矩阵Ck的第一行的前LC个元素组成的LC×1维向量;进而计算得到第k次修正后Q个入射信号的MUSIC谱值倒数和Jck,其计算表达式为:(4c) From the properties of the mutual coupling matrix of the uniform circular array described in (4b), it can be obtained that the mutual coupling matrix C k of the uniform circular array after the kth correction and the incident direction are The signal steering vector of Equivalent substitutions can be made, that is, Among them, c k is the LC × 1-dimensional vector composed of the first row of L C elements of the mutual coupling matrix C k of the uniform circular array after the k-th correction; then the Q incident signals after the k-th correction are calculated The reciprocal of the MUSIC spectrum value and J ck , the calculation expressions are:

其中,||||2表示取模值之后再求平方操作。in, |||| 2 means to calculate the square operation after taking the modulus value.

(4d)为了求解第k次修正后均匀圆阵的互耦矩阵Ck的第一行的前LC个元素组成的LC×1维向量ck,添加一个线性约束,假设均匀圆阵的互偶矩阵的阵元内部自阻抗为1,则Ck(1,1)=1,即eHck=1,其中e为首元素为1、其余元素均为0的L×1维向量,即建立如下方程:(4d) In order to solve the L C ×1-dimensional vector c k composed of the first L C elements of the first row of the mutual coupling matrix C k of the uniform circular array after the k-th correction, a linear constraint is added, assuming that the uniform circular array The internal self-impedance of the array element of the mutual dual matrix is 1, then C k (1,1) = 1, that is, e H c k = 1, where e is an L×1-dimensional vector whose first element is 1 and the rest of the elements are 0, That is, the following equation is established:

其中,上标H表示共轭转置操作,s.t.表示约束条件。Among them, the superscript H represents the conjugate transpose operation, and s.t. represents the constraint condition.

最后计算得到第k次修正后均匀圆阵的互耦矩阵Ck的第一行的前LC个元素组成的LC×1维向量ck,其表达式为:Finally, the LC × 1-dimensional vector c k composed of the first LC elements of the first line of the mutual coupling matrix C k of the uniform circular array after the k-th correction is calculated, and its expression is:

ck=Gk -1e(eHGk -1e)-1 c k =G k -1 e(e H G k -1 e) -1

由于第k次修正后均匀圆阵的互耦矩阵Ck的第一行的前LC个元素组成的LC×1维向量ck为第k次修正后均匀圆阵的互耦矩阵Ck的第一行的前LC个元素组成的LC×1维向量,且第k次修正后均匀圆阵的互耦矩阵Ck为一个复循环对称矩阵,故第k次修正后均匀圆阵的互耦矩阵Ck中的元素可以由第k次修正后均匀圆阵的互耦矩阵Ck的第一行的前LC个元素组成的LC×1维向量ck中元素完全确定。Since the mutual coupling matrix C k of the uniform circular array after the kth correction is the LC × 1-dimensional vector c k composed of the first LC elements of the first row of the uniform circular array, it is the mutual coupling matrix C k of the uniform circular array after the kth correction The LC × 1-dimensional vector composed of the first L C elements of the first row of , and the mutual coupling matrix C k of the uniform circular array after the k-th correction is a complex circular symmetric matrix, so the uniform circular array after the k-th correction The elements in the mutual coupling matrix C k can be completely determined by the elements in the LC ×1-dimensional vector c k composed of the first LC elements of the first row of the mutual coupling matrix C k of the uniform circular array after the kth correction.

因此,根据第k次修正后均匀圆阵的互耦矩阵Ck的第一行的前LC个元素组成的LC×1维向量ck,计算得到第k次修正后均匀圆阵的互耦矩阵CkTherefore, according to the LC × 1-dimensional vector c k composed of the first row of L C elements of the mutual coupling matrix C k of the uniform circular array after the kth correction, the mutual coupling matrix of the uniform circular array after the kth correction is calculated. Coupling matrix C k .

步骤5,令k加1,返回步骤3,直到Jck-Jc(k-1)<△,则修正迭代结束,Jc(k-1)表示第k-1次修正后Q个入射信号的MUSIC谱值倒数的和,△表示设定的门限值,本实施例中△取值为0.0001;并分别将修正迭代停止时对应的第k次修正后均匀圆阵的互耦矩阵Ck,记为均匀圆阵的最终互偶矩阵将修正迭代停止时对应的第k次修正后Q个入射信号的方位角θk,记为Q个入射信号的最终方位角 表示经过修正后第q+1个入射信号的最终方位角;进而得到Q个入射信号的Q个最终入射方向,分别为 φq表示第q+1个入射信号相对于均匀圆阵的俯仰角;其中,为期望信号的最终入射方向。Step 5, increase k by 1, return to step 3, until J ck -J c(k-1) <△, then the correction iteration ends, J c(k-1) represents the Q incident signals after the k-1th correction The sum of the reciprocals of the MUSIC spectrum values of , △ represents the set threshold value, and the value of △ in this embodiment is 0.0001; and the mutual coupling matrix C k of the uniform circular array corresponding to the kth correction when the correction iteration stops is respectively , denoted as the final mutual dual matrix of the uniform circular array The azimuth θ k of the Q incident signals corresponding to the k-th correction when the correction iteration stops is recorded as the final azimuth angle of the Q incident signals Indicates the final azimuth angle of the q+1th incident signal after correction; then the Q final incident directions of the Q incident signals are obtained, respectively: φ q represents the pitch angle of the q+1th incident signal relative to the uniform circular array; where, is the final incident direction of the desired signal.

步骤6,在已经获得Q个入射信号的Q个最终入射方向和均匀圆阵的最终互偶矩阵后开始进行均匀圆阵的干扰加噪声协方差矩阵重构;其中包括均匀圆阵的干扰协方差矩阵重构和均匀圆阵的噪声协方差矩阵重构;进而计算得到重构后均匀圆阵的干扰加噪声协方差矩阵。Step 6, after obtaining the Q final incident directions of Q incident signals and the final mutual dual matrix of the uniform circular array Then start to reconstruct the interference plus noise covariance matrix of the uniform circular array; including the reconstruction of the interference covariance matrix of the uniform circular array and the reconstruction of the noise covariance matrix of the uniform circular array; and then calculate the reconstructed uniform circular array Interference-plus-noise covariance matrix.

步骤6具体包括如下子步骤:Step 6 specifically includes the following sub-steps:

(6a)从Q个入射信号的Q个最终入射方向中剔除期望信号的最终入射方向中,获取Q-1个干扰信号的最终入射方向,分别为 (6a) Eliminate the final incident directions of the desired signal from the Q final incident directions of the Q incident signals, and obtain the final incident directions of Q-1 interference signals, respectively

考虑到谱估计算法的误差,设定方位角估计误差范围为△θ,这样Q-1个干扰信号角度区域可以表示为 Considering the error of the spectrum estimation algorithm, the azimuth estimation error range is set to △θ, so Q-1 interference signal angle regions can be expressed as

即Q-1个干扰信号的最终入射方向都位于内,且Q-1个干扰信号角度区域包含Q-1个离散采样点,每个离散采样点分别对应一个干扰信号的最终入射方向;在Q-1个干扰信号角度区域内任意选取L'个离散采样点计算协方差矩阵,L'≤Q-1,再进行求和得到重构后均匀圆阵的干扰协方差矩阵That is, the final incident directions of the Q-1 interference signals are located in In, and Q-1 interference signal angle area Contains Q-1 discrete sampling points, each discrete sampling point corresponds to the final incident direction of an interference signal; in the Q-1 interference signal angle area Randomly select L' discrete sampling points to calculate the covariance matrix, L'≤Q-1, and then sum to obtain the interference covariance matrix of the reconstructed uniform circular array which is

其中,∪表示求并集操作,b(θl'l')为Q-1个干扰信号角度区域内第l'个离散采样点处的导向矢量,l'=1,2,…,L',又根据Q个入射信号的Q个最终入射方向和均匀圆阵的最终互偶矩阵计算得到经过互耦校正后期望信号的导向矢量b(θ,φ),故计算得到重构后均匀圆阵的干扰协方差矩阵其表达式为:Among them, ∪ represents the union operation, b(θ l'l' ) is the Q-1 interference signal angle area The steering vector at the l'th discrete sampling point, l'=1,2,...,L', and according to the Q final incident directions of the Q incident signals and the final mutual-dual matrix of the uniform circular array Calculate the steering vector b(θ,φ) of the desired signal after mutual coupling correction, Therefore, the interference covariance matrix of the reconstructed uniform circular array is calculated Its expression is:

其中,R表示均匀圆阵的采样协方差矩阵,b(θl'l')表示Q-1个干扰信号角度区域内第l'个离散采样点处的导向矢量,与入射方向为(θl'l')的信号导向矢量取值相等;进而完成均匀圆阵的干扰协方差矩阵重构。Among them, R represents the sampling covariance matrix of the uniform circular array, and b(θ l' , φ l' ) represents Q-1 interference signal angle areas The steering vector at the l'th discrete sampling point within is equal to the signal steering vector with the incident direction (θ l' , φ l' ); then the interference covariance matrix reconstruction of the uniform circular array is completed.

(6b)进行均匀圆阵的噪声协方差矩阵重构,在理想状态下,对均匀圆阵的采样协方差矩阵进行特征分解后得到的M-Q个小特征值分别相等,其值就是噪声功率值。(6b) Reconstruct the noise covariance matrix of the uniform circular array. Under ideal conditions, the M-Q small eigenvalues obtained after eigendecomposition of the sampling covariance matrix of the uniform circular array are equal to each other, and their values are the noise power values.

但在实际情况中,M-Q个小特征值是不相等的,为了计算简便,在M-Q个小特征值选取特征值最小值,作为均匀圆阵的噪声功率估计值进而计算得到重构后均匀圆阵的噪声协方差矩阵I表示M×M维单位矩阵。But in the actual situation, the MQ small eigenvalues are not equal. For the sake of simplicity, the minimum value of the eigenvalue is selected from the MQ small eigenvalues as the noise power estimation value of the uniform circular array Then calculate the noise covariance matrix of the reconstructed uniform circular array I represents an M×M dimensional identity matrix.

(6c)进行均匀圆阵的干扰加噪声协方差矩阵重构:根据重构后均匀圆阵的干扰协方差矩阵和重构后均匀圆阵的噪声协方差矩阵计算得到重构后均匀圆阵的干扰加噪声协方差矩阵其表达式为:(6c) Reconstruct the interference plus noise covariance matrix of the uniform circular array: according to the interference covariance matrix of the uniform circular array after reconstruction and the noise covariance matrix of the reconstructed uniform circular array Calculate the interference plus noise covariance matrix of the reconstructed uniform circular array Its expression is:

其中,R表示均匀圆阵的采样协方差矩阵,I表示M×M维单位矩阵;进而完成了均匀圆阵的干扰加噪声协方差矩阵重构。Among them, R represents the sampling covariance matrix of the uniform circular array, and I represents the M×M dimensional unit matrix; then, the reconstruction of the interference-plus-noise covariance matrix of the uniform circular array is completed.

步骤7,计算得到期望信号的最终导向矢量为并根据重构后均匀圆阵的干扰加噪声协方差矩阵利用线性约束最小方差(LCMV)准则计算得到均匀圆阵的自适应波束形成器的权矢量为w,进而完成了基于迭代互耦校正的均匀圆阵干扰加噪声协方差矩阵重构的波束形成设计。Step 7, calculate the final steering vector of the desired signal as And according to the interference plus noise covariance matrix of the uniform circular array after reconstruction Using the linear constrained minimum variance (LCMV) criterion to calculate the weight vector of the adaptive beamformer of the uniform circular array is w, and then completed the beamforming design of the uniform circular array interference plus noise covariance matrix reconstruction based on iterative mutual coupling correction .

具体地,计算得到期望信号的最终导向矢量为 为入射方向为的信号导向矢量,为期望信号的最终入射方向,则利用线性约束最小方差(LCMV)准则求出均匀圆阵的自适应波束形成器的权矢量w,其表达式为:Specifically, the final steering vector of the desired signal is calculated as is the incident direction is The signal steering vector of , is the final incident direction of the desired signal, the weight vector w of the adaptive beamformer of the uniform circular array is obtained by using the linear constrained minimum variance (LCMV) criterion, and its expression is:

其中,上标-1表示求逆操作,上标H表示共轭转置操作;进而完成了基于迭代互耦校正的均匀圆阵干扰加噪声协方差矩阵重构的波束形成设计。Among them, the superscript -1 represents the inversion operation, and the superscript H represents the conjugate transposition operation; and then the beamforming design of the uniform circular array interference plus noise covariance matrix reconstruction based on iterative mutual coupling correction is completed.

通过以下仿真实验对本发明效果作进一步验证说明。The effects of the present invention are further verified and illustrated by the following simulation experiments.

(一)仿真条件(1) Simulation conditions

本发明的仿真实验在MATLAB软件下进行的,在本发明的实验中,均匀圆阵采用10个阵元,Q个入射信号的信号波长设置为0.1米,相邻阵元间距d与Q个入射信号的信号波长的比值d/λ的为0.5,每个入射信号相对于均匀圆阵的俯仰角均设置为30°,期望信号的方位角设置为95°,设置两个干扰信号,两个干扰信号的方位角分别为50°和140°。The simulation experiment of the present invention is carried out under MATLAB software, and in the experiment of the present invention, uniform circular array adopts 10 array elements, and the signal wavelength of Q incident signal is set to 0.1 meter, and adjacent array element spacing d and Q incident The signal wavelength ratio d/λ of the signal is 0.5, the pitch angle of each incident signal relative to the uniform circular array is set to 30°, the azimuth angle of the desired signal is set to 95°, two interference signals are set, and two interference signals The azimuth angles of the signals are 50° and 140°, respectively.

具体的算法参数如下表所示:The specific algorithm parameters are shown in the table below:

(二)仿真内容和结果分析(2) Simulation content and result analysis

为了说明本发明算法的优越性,图2到图5给出了其他几种波束形成算法的处理结果,包括最优波束形成器,采样矩阵求逆(SMI)波束形成器,协方差矩阵重构算法和最差性能最优化方法。In order to illustrate the superiority of the algorithm of the present invention, Figures 2 to 5 show the processing results of several other beamforming algorithms, including optimal beamformers, sampling matrix inversion (SMI) beamformers, and covariance matrix reconstruction Algorithms and worst-case performance optimization methods.

图2的横轴表示输入信噪比,纵轴表示输出信干噪比;图2表示存在信号观测误差,采样快拍数为30,几种波束形成方法的输出信干噪比随期望信号输入信干噪比变化的曲线。从图2中我们可以看到,在同时存在互耦影响和入射信号观测误差的情况下,普通协方差矩阵重构方法性能急剧下降,在低信噪比的场景中性能甚至远远不如SMI方法;最差性能最优化波束形成方法保有较好的性能稳健性,但是在期望信号功率变强时其性能与理论最优值的差距在增大;而本发明提出的基于互耦校正的协方差矩阵重构方法在高信噪比条件下性能极为接近理论最优值,在低信噪比条件下算法的性能有所下降,这是因为在期望信号功率低于噪声水平时,DOA估计会发生失准,从而影响波束形成器的性能。The horizontal axis in Fig. 2 represents the input SNR, and the vertical axis represents the output SINR; Fig. 2 shows that there are signal observation errors, the number of sampling snapshots is 30, and the output SINR of several beamforming methods varies with the expected signal input The curve of the signal-to-interference-to-noise ratio change. From Figure 2, we can see that in the presence of mutual coupling effects and incident signal observation errors, the performance of the ordinary covariance matrix reconstruction method drops sharply, and the performance in low signal-to-noise ratio scenarios is even far inferior to the SMI method ; The worst performance optimization beamforming method maintains better performance robustness, but when the expected signal power becomes stronger, the gap between its performance and the theoretical optimal value is increasing; and the covariance based on mutual coupling correction proposed by the present invention The performance of the matrix reconstruction method is very close to the theoretical optimal value under the condition of high signal-to-noise ratio, and the performance of the algorithm decreases under the condition of low signal-to-noise ratio, because the DOA estimation will occur when the expected signal power is lower than the noise level misalignment, thereby affecting the performance of the beamformer.

图3(a)和图3(b)的横轴表示采样样本数,纵轴表示波束形成器的输出信干噪比;图3(a)表示在存在信号观测误差且输入信噪比为20dB时的仿真结果,图3(b)表示在存在信号观测误差且输入信噪比为-5dB时的仿真结果。仿真结果表明,在期望信号的输入信噪比比较高时,本发明所提出的波束形成方法性能大幅优越于其他波束形成方法;在低信噪比的情况下如果能够保证样本充足,本发明提出的波束形成算法仍然具有很好的性能。The horizontal axis of Figure 3(a) and Figure 3(b) represents the number of sampling samples, and the vertical axis represents the output signal-to-interference-noise ratio of the beamformer; Figure 3(a) shows that there is a signal observation error and the input signal-to-noise ratio is 20dB Figure 3(b) shows the simulation results when there are signal observation errors and the input signal-to-noise ratio is -5dB. Simulation results show that when the input signal-to-noise ratio of the desired signal is relatively high, the performance of the beamforming method proposed by the present invention is significantly superior to other beamforming methods; The beamforming algorithm still has very good performance.

图4的横轴表示输入信噪比,纵轴表示输出信干噪比;图4表示不存在信号观测误差,采样快拍数为30,几种波束形成方法的输出信干噪比随期望信号输入信干噪比变化的曲线。从图4中我们可以看到,在只考虑均匀圆阵的互耦造成期望信号和干扰信号导向矢量失配的条件下,经过本方法互耦校正后,波束形成器的性能在高信噪比情况下与理论最优值几乎没有差距,这是因为本方法只针对互耦因素进行校正,并且剔除了采样协方差矩阵中的期望信号分量,在不考虑其他失配因素的情况下可以达到接近理论最优的性能。The horizontal axis of Fig. 4 represents the input SNR, and the vertical axis represents the output SINR; Fig. 4 shows that there is no signal observation error, the number of sampling snapshots is 30, and the output SINR of several beamforming methods varies with the expected signal Input the curve of SINR change. From Figure 4, we can see that under the condition that only the mutual coupling of the uniform circular array is considered to cause the steering vector mismatch between the desired signal and the interference signal, after the mutual coupling correction by this method, the performance of the beamformer is at a high SNR In this case, there is almost no gap with the theoretical optimal value, because this method only corrects for mutual coupling factors, and eliminates the expected signal component in the sampling covariance matrix, and can achieve close to Theoretical optimal performance.

图5(a)和图5(b)的横轴表示采样样本数,纵轴表示波束形成器的输出信干噪比;图5(a)表示不存在信号观测误差且输入信噪比为20dB时的仿真结果,图3(b)表示不存在信号观测误差且输入信噪比为-5dB时的仿真结果。结果表明,在职考虑均匀圆阵的互耦造成期望信号和干扰信号导向矢量失配的条件下,本发明方法的性能相比考虑了信号观测误差是要好一些。The horizontal axis of Figure 5(a) and Figure 5(b) represents the number of sampling samples, and the vertical axis represents the output signal-to-interference-noise ratio of the beamformer; Figure 5(a) shows that there is no signal observation error and the input signal-to-noise ratio is 20dB Figure 3(b) shows the simulation results when there is no signal observation error and the input signal-to-noise ratio is -5dB. The results show that under the condition that the mutual coupling of the uniform circular array is considered, the performance of the method of the present invention is better than that of the signal observation error.

综上所述,仿真实验验证了本发明的正确性,有效性和可靠性。In summary, the simulation experiment has verified the correctness, effectiveness and reliability of the present invention.

以上所述,仅为本发明的具体实施方式,但本发明的保护范围并不局限于此,任何熟悉本技术领域的技术人员在本发明揭露的技术范围内,可轻易想到变化或替换,都应涵盖在本发明的保护范围之内。因此,本发明的保护范围应以所述权利要求的保护范围为准。The above is only a specific embodiment of the present invention, but the scope of protection of the present invention is not limited thereto. Anyone skilled in the art can easily think of changes or substitutions within the technical scope disclosed in the present invention. Should be covered within the protection scope of the present invention. Therefore, the protection scope of the present invention should be determined by the protection scope of the claims.

Claims (4)

1.一种基于迭代互耦校正的雷达协方差矩阵重构波束形成方法,其特征在于,包括以下步骤:1. A radar covariance matrix reconstruction beamforming method based on iterative mutual coupling correction, is characterized in that, comprises the following steps: 步骤1,确定均匀圆阵,该均匀圆阵包括M个阵元,均匀圆阵设定范围内存在Q个信号源,Q个信号源向均匀圆阵发射Q个入射信号,所述Q个入射信号包含1个期望信号和Q-1个干扰信号;Step 1, determine the uniform circular array, the uniform circular array includes M array elements, there are Q signal sources within the set range of the uniform circular array, and the Q signal sources transmit Q incident signals to the uniform circular array, and the Q incident signals The signal contains 1 desired signal and Q-1 interference signals; 获取均匀圆阵的采样协方差矩阵R,并对所述均匀圆阵的采样协方差矩阵R进行特征分解,得到M个特征值;M、Q分别为大于0的正整数,Q>1,M表示均匀圆阵包括的阵元个数,与对均匀圆阵的采样协方差矩阵R进行特征分解后得到的特征值个数取值相等;Obtain the sampling covariance matrix R of the uniform circular array, and perform eigendecomposition on the sampling covariance matrix R of the uniform circular array to obtain M eigenvalues; M and Q are positive integers greater than 0, Q>1, M Indicates the number of array elements included in the uniform circular array, which is equal to the number of eigenvalues obtained after eigendecomposing the sampling covariance matrix R of the uniform circular array; 步骤2,计算入射方向为(θ,φ)的信号MUSIC谱,然后设定均匀圆阵的互耦矩阵初始值,进而得到Q个入射信号的Q个方位角初始值,分别为q∈{0,1,2,…,Q-1},表示第q+1个入射信号的方位角初始值;Step 2, calculate the MUSIC spectrum of the signal with the incident direction (θ, φ), and then set the initial value of the mutual coupling matrix of the uniform circular array, and then obtain the initial values of Q azimuth angles of the Q incident signals, respectively q ∈ {0,1,2,...,Q-1}, Indicates the initial value of the azimuth angle of the q+1th incident signal; 初始化:令k表示第k次修正,k的初始值为1;令第k次修正后均匀圆阵的互耦矩阵为Ck,并将Q个入射信号的Q个方位角初始值作为第0次修正后Q个入射信号的方位角θ0;设定均匀圆阵的互耦矩阵初始值为C0,C0=IM,IM表示M×M维单位矩阵;Initialization: let k represent the kth correction, and the initial value of k is 1; let the mutual coupling matrix of the uniform circular array after the kth correction be C k , and set the initial values of Q azimuth angles of the Q incident signals as the 0th The azimuth angle θ 0 of the Q incident signals after the second correction; the initial value of the mutual coupling matrix of the uniform circular array is set to C 0 , C 0 =I M , and I M represents the M×M dimensional identity matrix; 步骤3,根据第k次修正后均匀圆阵的互耦矩阵Ck对Q个入射信号分别进行波达方向估计,得到第k次修正后入射方向为(θk,φ)的信号MUSIC谱PMUSICk,φ),以及第k次修正后Q个入射信号的方位角;Step 3: According to the mutual coupling matrix C k of the uniform circular array after the k-th correction, the direction of arrival is estimated for the Q incident signals respectively, and the MUSIC spectrum P of the signal whose incident direction is (θ k , φ) after the k-th correction is obtained MUSICk ,φ), and the azimuth angles of the Q incident signals after the kth correction; 步骤4,依次得到第k次修正后Q个入射信号的MUSIC谱值倒数的和Jck的定义式和计算式,进而计算得到第k次修正后均匀圆阵的互耦矩阵CkStep 4, sequentially obtain the definition formula and calculation formula of the reciprocal sum J ck of the MUSIC spectrum values of the Q incident signals after the k-th correction, and then calculate the mutual coupling matrix C k of the uniform circular array after the k-th correction; 步骤5,令k加1,返回步骤3,直到Jck-Jc(k-1)<Δ,则修正迭代结束,Jc(k-1)表示第k-1次修正后Q个入射信号的MUSIC谱值倒数的和,Δ表示设定的门限值,并分别将修正迭代停止时对应的第k次修正后均匀圆阵的互耦矩阵Ck,记为均匀圆阵的最终互偶矩阵将修正迭代停止时对应的第k次修正后Q个入射信号的方位角,记为Q个入射信号的最终方位角 Step 5, increase k by 1, and return to step 3 until J ck -J c(k-1) <Δ, then the correction iteration ends, and J c(k-1) represents the Q incident signals after the k-1th correction The sum of the reciprocals of the MUSIC spectrum values of , Δ represents the set threshold value, and the mutual coupling matrix C k of the uniform circular array corresponding to the kth correction when the correction iteration stops is recorded as the final mutual coupling matrix of the uniform circular array matrix The azimuth angles of the Q incident signals corresponding to the kth correction when the correction iteration stops are recorded as the final azimuth angles of the Q incident signals 步骤6,根据均匀圆阵的最终互偶矩阵和Q个入射信号的最终方位角计算得到重构后均匀圆阵的干扰加噪声协方差矩阵 Step 6, according to the final mutual dual matrix of the uniform circular array and the final azimuths of the Q incident signals Calculate the interference plus noise covariance matrix of the reconstructed uniform circular array 步骤7,计算得到期望信号的最终导向矢量,并根据重构后均匀圆阵的干扰加噪声协方差矩阵计算得到均匀圆阵的自适应波束形成器的权矢量为w,进而完成了基于迭代互耦校正的均匀圆阵干扰加噪声协方差矩阵重构的波束形成设计;Step 7, calculate the final steering vector of the desired signal, and according to the interference-plus-noise covariance matrix of the reconstructed uniform circular array The weight vector of the adaptive beamformer of the uniform circular array is calculated as w, and then the beamforming design of the uniform circular array interference plus noise covariance matrix reconstruction based on iterative mutual coupling correction is completed; 其中,在步骤1中,所述Q个入射信号,还包括:Wherein, in step 1, the Q incident signals also include: Q个入射信号相对于均匀圆阵的俯仰角为φ,φ={φ01,…,φq,…,φQ-1},q∈{0,1,…,Q-1},φq表示第q+1个入射信号相对于均匀圆阵的俯仰角,且φ0、φ1、…、φq、…、φQ-1取值分别相等;φ0表示期望信号相对于均匀圆阵的俯仰角,Q-1个干扰信号相对于均匀圆阵的俯仰角分别为φ1、φ2、…、φQ-1The pitch angle of the Q incident signals relative to the uniform circular array is φ, φ={φ 01 ,…,φ q ,…,φ Q-1 }, q∈{0,1,…,Q-1} , φ q represents the pitch angle of the q+1th incident signal relative to the uniform circular array, and the values of φ 0 , φ 1 , ..., φ q , ..., φ Q-1 are equal; φ 0 represents the desired signal relative to The pitch angle of the uniform circular array, the pitch angles of the Q-1 interference signals relative to the uniform circular array are φ 1 , φ 2 , ..., φ Q-1 respectively; 对所述均匀圆阵的采样协方差矩阵R进行特征分解,其分解形式为:Carry out eigendecomposition to the sampling covariance matrix R of described uniform circular array, its decomposition form is: 其中,R为均匀圆阵的采样协方差矩阵,维数为M×M;ΛSI为Q个大特征值分别为对角元素形成的对角矩阵,USI为Q个大特征值对应的特征向量形成的期望信号加干扰子空间,ΛN为M-Q个小特征值分别为对角元素形成的对角矩阵,UN为M-Q个小特征值对应的特征向量形成的噪声子空间,上标H表示共轭转置操作,M、Q分别为大于0的正整数,M>Q;M表示均匀圆阵包括的阵元个数,与对均匀圆阵的采样协方差矩阵R进行特征分解后得到的特征值个数取值相等;Among them, R is the sampling covariance matrix of the uniform circular array, and its dimension is M×M; Λ SI is a diagonal matrix formed by the Q large eigenvalues respectively being diagonal elements, and U SI is the characteristic corresponding to the Q large eigenvalues The desired signal plus interference subspace formed by the vector, Λ N is a diagonal matrix formed by MQ small eigenvalues respectively as diagonal elements, U N is the noise subspace formed by the eigenvectors corresponding to MQ small eigenvalues, superscript H Represents the conjugate transposition operation, M and Q are positive integers greater than 0, M>Q; M represents the number of array elements included in the uniform circular array, which is obtained by performing eigendecomposition on the sampling covariance matrix R of the uniform circular array The number of eigenvalues of is equal; 在步骤2中,所述入射方向为(θ,φ)的信号MUSIC谱PMUSIC(θ,φ),其表达式为:In step 2, said incident direction is the signal MUSIC spectrum P MUSIC (θ, φ) of (θ, φ), its expression is: 其中,θ表示Q个入射信号的方位角,φ表示Q个入射信号相对于均匀圆阵的俯仰角,a(θ,φ)为入射方向为(θ,φ)的信号导向矢量,C为均匀圆阵的互耦矩阵,UN为M-Q个小特征值对应的特征向量形成的噪声子空间,上标H表示共轭转置操作;Among them, θ represents the azimuth angle of the Q incident signals, φ represents the elevation angle of the Q incident signals relative to the uniform circular array, a(θ, φ) is the signal steering vector with the incident direction (θ, φ), and C is the uniform The mutual coupling matrix of the circular array, U N is the noise subspace formed by the eigenvectors corresponding to MQ small eigenvalues, and the superscript H represents the conjugate transpose operation; 所述得到Q个入射信号的Q个方位角初始值,其过程为:The process of obtaining Q initial values of Q azimuth angles of Q incident signals is as follows: 设定均匀圆阵的互耦矩阵初始值C0,C0=IM,IM表示M×M维单位矩阵;将均匀圆阵的互耦矩阵初始值C0代入入射方向为(θ,φ)的信号MUSIC谱PMUSIC(θ,φ)表达式中,并在0°到180°方位角范围内搜索MUSIC谱峰,进而得到Q个入射信号的Q个方位角初始值,分别为q∈{0,1,2,…,Q-1},表示第q+1个入射信号的方位角初始值;其中,设定方位角范围内为0°到180°范围内;Set the initial value C 0 of the mutual coupling matrix of the uniform circular array, C 0 =I M , I M represents the M×M dimensional unit matrix; substitute the initial value C 0 of the mutual coupling matrix of the uniform circular array into the incident direction as (θ,φ ) signal MUSIC spectrum P MUSIC (θ, φ) expression, and search the MUSIC spectrum peak in the range of 0° to 180° azimuth angle, and then get the initial values of Q azimuth angles of Q incident signals, respectively q ∈ {0,1,2,...,Q-1}, Indicates the initial value of the azimuth angle of the q+1th incident signal; wherein, the set azimuth angle range is within the range of 0° to 180°; 在步骤3中,所述第k次修正后入射方向为(θk,φ)的信号MUSIC谱PMUSICk,φ),其表达式为:In step 3, the signal MUSIC spectrum P MUSICk , φ) whose incident direction is (θ k , φ) after the kth correction is expressed as: 其中,θk表示第k次修正后Q个入射信号的方位角,φ表示Q个入射信号相对于均匀圆阵的俯仰角,a(θk,φ)为入射方向为(θk,φ)的信号导向矢量,Ck为第k次修正后均匀圆阵的互耦矩阵,UN为M-Q个小特征值对应的特征向量形成的噪声子空间,上标H表示共轭转置操作;Among them, θ k represents the azimuth angle of the Q incident signals after the kth correction, φ represents the elevation angle of the Q incident signals relative to the uniform circular array, and a(θ k , φ) is the incident direction as (θ k , φ) The signal steering vector of , C k is the mutual coupling matrix of the uniform circular array after the kth correction, U N is the noise subspace formed by the eigenvectors corresponding to MQ small eigenvalues, and the superscript H represents the conjugate transpose operation; 在设定方位角范围内搜索第k次修正后入射方向为(θk,φ)的信号MUSIC谱PMUSICk,φ)的MUSIC谱峰,得到第k次修正后Q个入射信号的方位角为θk,θk={θ0k1k,…,θqk,…,θ(Q-1)k},q∈{0,1,…,Q-1},θqk表示第k次修正后第q+1个入射信号的方位角;θ0k表示第k次修正后期望信号的方位角,θ1k2k,…,θ(Q-1)k为第k次修正后Q-1个干扰信号的方位角;其中,设定方位角范围内为0°到180°范围内;Search for the MUSIC spectrum peak of the signal MUSIC spectrum P MUSICk , φ) with the incident direction (θ k , φ) after the k-th correction within the range of the set azimuth angle, and obtain the MUSIC spectrum peak of the Q incident signal after the k-th correction The azimuth angle is θ k , θ k ={θ 0k1k ,…,θ qk ,…,θ (Q-1)k }, q∈{0,1,…,Q-1}, θ qk represents the The azimuth angle of the q+1th incident signal after the k-th correction; θ 0k represents the azimuth angle of the expected signal after the k-th correction, θ 1k , θ 2k ,…, θ (Q-1)k is the k-th correction The azimuth angle of Q-1 interference signal; wherein, the set azimuth angle range is within the range of 0° to 180°; 步骤4的子步骤为:The sub-steps of step 4 are: (4a)根据第k次修正后均匀圆阵的互耦矩阵Ck,定义第k次修正后Q个入射信号的MUSIC谱值倒数的和为Jck,其定义表达式为:(4a) According to the mutual coupling matrix C k of the uniform circular array after the k-th correction, the sum of the reciprocals of the MUSIC spectrum values of the Q incident signals after the k-th correction is defined as J ck , and the definition expression is: 其中,表示入射方向为的信号导向矢量,φq表示第q+1个入射信号相对于均匀圆阵的俯仰角, 表示第k次修正后第q+1个入射信号的方位角,|| ||2表示取模值之后再求平方操作;Ck为第k次修正后均匀圆阵的互耦矩阵,UN为M-Q个小特征值对应的特征向量形成的噪声子空间,上标H表示共轭转置操作;in, Indicates that the direction of incidence is The signal steering vector of , φ q represents the pitch angle of the q+1th incident signal relative to the uniform circular array, Indicates the azimuth angle of the q+1th incident signal after the kth correction, || || 2 represents the square operation after taking the modulus value; C k is the mutual coupling matrix of the uniform circular array after the kth correction, U N is the noise subspace formed by the eigenvectors corresponding to MQ small eigenvalues, and the superscript H represents the conjugate transpose operation; (4b)确定第k次修正后均匀圆阵的互耦矩阵Ck由第k次修正后均匀圆阵的互耦矩阵Ck第一行中的前LC个元素完全确定, 表示向下取整操作;并且确定第k次修正后均匀圆阵的互耦矩阵Ck与入射方向为(θk,φ)的信号导向矢量a(θk,φ)的乘积,等价于入射方向为(θk,φ)的信号导向矢量a(θk,φ)中的M个元素组成的M×LC维矩阵Q[a(θk,φ)]与第k次修正后均匀圆阵的互耦矩阵Ck中第一行的前LC个元素完组成的LC×1维向量ck的乘积,即Cka(θk,φ)=Q[a(θk,φ)]ck(4b) Determine the mutual coupling matrix C k of the uniform circular array after the k-th correction is completely determined by the first L C elements in the first row of the mutual coupling matrix C k of the uniform circular array after the k-th correction, Represents the rounding down operation; and determine the product of the mutual coupling matrix C k of the uniform circular array after the kth correction and the signal steering vector a(θ k , φ) with the incident direction (θ k , φ), which is equivalent to The M×L C -dimensional matrix Q[a(θ k ,φ)] composed of M elements in the signal steering vector a(θ k ,φ) with the incident direction (θ k ,φ) is equal to The product of LC × 1-dimensional vector c k formed by the first LC elements of the first row in the mutual coupling matrix C k of the circular array, that is, C k a(θ k ,φ)=Q[a(θ k , φ)] c k ; 其中,ck为第k次修正后均匀圆阵的互耦矩阵Ck中第一行的前LC个元素组成的LC×1维向量,d∈{0,1,…,LC-1},cdk表示第k次修正后均匀圆阵的互耦矩阵Ck中第一行的第d+1个元素,上标T表示转置操作;Among them, c k is the LC × 1-dimensional vector composed of the first LC elements in the first row of the mutual coupling matrix C k of the uniform circular array after the k-th correction, d∈{0,1,…,L C -1}, c dk represents the d+1th element in the first row of the mutual coupling matrix C k of the uniform circular array after the k-th correction, and the superscript T represents the transpose operate; 入射方向为(θk,φ)的信号导向矢量a(θk,φ)中的M个元素组成的M×LC维矩阵Q[a(θk,φ)]由第k次修正后的第一M×LC维矩阵Q1k、第k次修正后的第二M×LC维矩阵Q2k、第k次修正后的第三M×LC维矩阵Q3k和第k次修正后的第四M×LC维矩阵Q4k相加得到,即Q[a(θk,φ)]=Q1k+Q2k+Q3k+Q4k,第k次修正后的第一M×LC维矩阵Q1k、第k次修正后的第二M×LC维矩阵Q2k、第k次修正后的第三M×LC维矩阵Q3k和第k次修正后的第四M×LC维矩阵Q4k分别由入射方向为(θk,φ)的信号导向矢量a(θk,φ)中的元素构成,其中第k次修正后的第一M×LC维矩阵Q1k中第r行、第h列元素为Q1(r,h)k,第k次修正后的第二M×LC维矩阵Q2k中第r'行、第h'列元素为Q2(r',h')k,第k次修正后的第三M×LC维矩阵Q3中第r”行、第h”列元素为Q3(r”,h”)k,第k次修正后的第四M×LC维矩阵Q4中第r”'行、第h”'列元素为Q4(r”',h”')k,表达式分别为:The M×L C -dimensional matrix Q[a(θ k ,φ)] composed of M elements in the signal steering vector a(θ k ,φ) with the incident direction (θ k ,φ) is modified by the kth The first M×L C -dimensional matrix Q 1k , the second M×L C -dimensional matrix Q 2k after the k-th correction, the third M×L C -dimensional matrix Q 3k after the k-th correction, and the k-th correction The fourth M×L C -dimensional matrix Q 4k is obtained by adding, that is, Q[a(θ k ,φ)]=Q 1k +Q 2k +Q 3k +Q 4k , the first M×L after the kth correction C -dimensional matrix Q 1k , the second M×L C -dimensional matrix Q 2k after the k-th correction, the third M×L C -dimensional matrix Q 3k after the k-th correction, and the fourth M×L C-dimensional matrix Q 3k after the k-th correction The L C -dimensional matrix Q 4k is composed of the elements in the signal-steering vector a(θ k , φ) with the incident direction (θ k , φ), where the first M×L C -dimensional matrix Q 1k after the kth correction The element in row r and column h in is Q 1(r,h)k , and the element in row r' and column h' in the second M×L C -dimensional matrix Q 2k after the kth correction is Q 2( r',h')k , the third M×L C -dimensional matrix Q 3 after the k-th correction, the elements in the r"th row and the h"th column are Q 3(r",h")k , the k-th The element in row r"' and column h"' in the fourth M×L C -dimensional matrix Q 4 after modification is Q 4(r"',h"')k , and the expressions are respectively: 其中,r∈{1,2,…,row1k},h∈{1,2,…,col1k},row1k表示第k次修正后的第一M×LC维矩阵Q1k的行数,col1k表示第k次修正后的第一M×LC维矩阵Q1k的列数,r'∈{1,2,…,row2k},h'∈{1,2,…,col2k},row2k表示第k次修正后的第二M×LC维矩阵Q2k的行数,col2k表示第k次修正后的第二M×LC维矩阵Q2k的列数,r”∈{1,2,…,row3k},h”∈{1,2,…,col3k},row3k表示第k次修正后的第三M×LC维矩阵Q3k的行数,col3k表示第k次修正后的第三M×LC维矩阵Q3k的列数,r”'∈{1,2,…,row4k},h”'∈{1,2,…,col4k},row4k表示第k次修正后的第四M×LC维矩阵Q4k的行数,col4k表示第k次修正后的第四M×LC维矩阵Q4k的列数, 表示向上取整操作;a(θk,φ)r+h-1表示入射方向为(θk,φ)的信号导向矢量a(θk,φ)中第r+h-1个元素,a(θk,φ)r'-h'+1表示入射方向为(θk,φ)的信号导向矢量a(θk,φ)中第r'-h'+1个元素,a(θk,φ)M+1+r”-h”表示入射方向为(θk,φ)的信号导向矢量a(θk,φ)中第M+1+r”-h”个元素,a(θk,φ)r”'+h”'-M-1表示入射方向为(θk,φ)的信号导向矢量a(θk,φ)中第r”'+h”'-M-1个元素;θk表示第k次修正后Q个入射信号的方位角,且第0次修正后Q个入射信号的方位角θ0为Q个入射信号的Q个方位角初始值;Among them, r∈{1,2,…,row 1k }, h∈{1,2,…,col 1k }, row 1k represents the number of rows of the first M×L C -dimensional matrix Q 1k after the kth correction , col 1k represents the number of columns of the first M×L C -dimensional matrix Q 1k after the kth correction, r'∈{1,2,...,row 2k }, h'∈{1,2,...,col 2k }, row 2k represents the row number of the second M×L C -dimensional matrix Q 2k after the k-th correction, col 2k represents the column number of the second M×L C -dimensional matrix Q 2k after the k-th correction, r” ∈{1,2,…,row 3k }, h”∈{1,2,…,col 3k }, row 3k represents the number of rows of the third M×L C -dimensional matrix Q 3k after the kth correction, col 3k represents the number of columns of the third M×L C -dimensional matrix Q 3k after the kth correction, r"'∈{1,2,...,row 4k }, h"'∈{1,2,...,col 4k }, row 4k represents the number of rows of the fourth M×L C -dimensional matrix Q 4k after the k correction, and col 4k represents the column number of the fourth M×L C -dimensional matrix Q 4k after the k correction, Represents an upward rounding operation; a(θ k ,φ) r+h-1 represents the r+h-1th element in the signal steering vector a(θ k ,φ) with the incident direction (θ k ,φ), a (θ k ,φ) r'-h'+1 represents the r'-h'+1th element in the signal steering vector a(θ k ,φ) with the incident direction (θ k ,φ), a(θ k ,φ) M+1+r”-h” represents the M+1+r”-h”th element in the signal steering vector a(θ k ,φ) with the incident direction (θ k ,φ), a(θ k , φ) r"'+h"'-M-1 means the r"'+h"'-M-1 of the signal steering vector a(θ k ,φ) with the incident direction (θ k ,φ) element; θ k represents the azimuth angles of the Q incident signals after the kth correction, and the azimuth angles θ of the Q incident signals after the 0th correction are the initial values of the Q azimuth angles of the Q incident signals; (4c)确定第k次修正后的均匀圆阵的互耦矩阵Ck与入射方向为的信号导向矢量进行等价代换,即其中,ck为第k次修正后均匀圆阵的互耦矩阵Ck的第一行的前LC个元素组成的LC×1维向量;进而计算得到第k次修正后Q个入射信号的MUSIC谱值倒数和Jck,其计算表达式为:(4c) Determine the mutual coupling matrix C k of the uniform circular array after the kth correction and the incident direction as The signal steering vector of perform an equivalent substitution, that is, Among them, c k is the LC × 1-dimensional vector composed of the first row of L C elements of the mutual coupling matrix C k of the uniform circular array after the k-th correction; then the Q incident signals after the k-th correction are calculated The reciprocal of the MUSIC spectrum value and J ck , the calculation expressions are: 其中,|| ||2表示取模值之后再求平方操作;in, || || 2 means to calculate the square operation after taking the modulus value; (4d)建立如下方程:(4d) Establish the following equation: 其中,e为首元素为1、其余元素均为0的L×1维向量,上标H表示共轭转置操作,s.t.表示约束条件;Among them, e is an L×1-dimensional vector whose first element is 1 and the rest of the elements are 0, the superscript H indicates the conjugate transpose operation, and s.t. indicates the constraint condition; 然后计算得到第k次修正后均匀圆阵的互耦矩阵Ck的第一行的前LC个元素组成的LC×1维向量ck,其表达式为:Then calculate the LC × 1-dimensional vector c k composed of the first LC elements of the first line of the mutual coupling matrix C k of the uniform circular array after the kth correction, and its expression is: ck=Gk -1e(eHGk -1e)-1 c k =G k -1 e(e H G k -1 e) -1 最后根据第k次修正后均匀圆阵的互耦矩阵Ck的第一行的前LC个元素组成的LC×1维向量ck,计算得到第k次修正后均匀圆阵的互耦矩阵CkFinally, according to the LC × 1-dimensional vector c k composed of the first LC elements of the first row of the mutual coupling matrix C k of the uniform circular array after the k-th correction, the mutual coupling of the uniform circular array after the k-th correction is calculated Matrix C k . 2.如权利要求1所述的一种基于迭代互耦校正的雷达协方差矩阵重构波束形成方法,其特征在于,在步骤5中,所述Q个入射信号的最终方位角具体为:2. A kind of radar covariance matrix reconstruction beamforming method based on iterative mutual coupling correction as claimed in claim 1, is characterized in that, in step 5, the final azimuth angle of the Q incident signals Specifically: Q个入射信号的最终方位角 表示经过修正后第q+1个入射信号的最终方位角;进而得到Q个入射信号的Q个最终入射方向,分别为φq表示第q+1个入射信号相对于均匀圆阵的俯仰角;其中,为期望信号的最终入射方向。Final azimuth of Q incident signals Indicates the final azimuth angle of the q+1th incident signal after correction; then the Q final incident directions of the Q incident signals are obtained, respectively: φ q represents the pitch angle of the q+1th incident signal relative to the uniform circular array; where, is the final incident direction of the desired signal. 3.如权利要求2所述的一种基于迭代互耦校正的雷达协方差矩阵重构波束形成方法,其特征在于,在步骤6中,所述重构后均匀圆阵的干扰加噪声协方差矩阵其得到过程为:3. A kind of radar covariance matrix reconstruction beamforming method based on iterative mutual coupling correction as claimed in claim 2, is characterized in that, in step 6, the interference of the uniform circular array after the reconstruction adds the noise covariance matrix Its obtaining process is: (6a)从Q个入射信号的Q个最终入射方向中剔除期望信号的最终入射方向中,获取Q-1个干扰信号的最终入射方向,分别为 (6a) Eliminate the final incident directions of the desired signal from the Q final incident directions of the Q incident signals, and obtain the final incident directions of Q-1 interference signals, respectively 设定方位角估计误差范围为Δθ,并将Q-1个干扰信号角度区域表示为 Set the azimuth estimation error range to Δθ, and express the Q-1 interference signal angle areas as 所述Q-1个干扰信号的最终入射方向都位于内,且Q-1个干扰信号角度区域包含Q-1个离散采样点,每个离散采样点分别对应一个干扰信号的最终入射方向;在Q-1个干扰信号角度区域内任意选取L'个离散采样点计算协方差矩阵,L'≤Q-1,再进行求和得到重构后均匀圆阵的干扰协方差矩阵其表达式为:The final incident directions of the Q-1 interference signals are located in In, and Q-1 interference signal angle area Contains Q-1 discrete sampling points, each discrete sampling point corresponds to the final incident direction of an interference signal; in the Q-1 interference signal angle area Randomly select L' discrete sampling points to calculate the covariance matrix, L'≤Q-1, and then sum to obtain the interference covariance matrix of the reconstructed uniform circular array Its expression is: 其中,∪表示求并集操作,b(θl'l')为Q-1个干扰信号角度区域内第l'个离散采样点处的导向矢量,与入射方向为(θl'l')的信号导向矢量取值相等;l'=1,2,…,L';Among them, ∪ represents the union operation, b(θ l'l' ) is the Q-1 interference signal angle area The steering vector at the l'th discrete sampling point within is equal to the value of the signal steering vector with the incident direction (θ l' , φ l' ); l'=1,2,...,L'; (6b)计算得到重构后均匀圆阵的噪声协方差矩阵I表示M×M维单位矩阵;其中,表示均匀圆阵的噪声功率估计值;(6b) Calculate the noise covariance matrix of the reconstructed uniform circular array I represents the M×M dimensional identity matrix; where, Indicates the noise power estimate of the uniform circular array; (6c)根据重构后均匀圆阵的干扰协方差矩阵和重构后均匀圆阵的噪声协方差矩阵计算得到重构后均匀圆阵的干扰加噪声协方差矩阵其表达式为:(6c) According to the interference covariance matrix of the uniform circular array after reconstruction and the noise covariance matrix of the reconstructed uniform circular array Calculate the interference plus noise covariance matrix of the reconstructed uniform circular array Its expression is: 其中,R表示均匀圆阵的采样协方差矩阵,I表示M×M维单位矩阵。Among them, R represents the sampling covariance matrix of the uniform circular array, and I represents the M×M dimensional identity matrix. 4.如权利要求3所述的一种基于迭代互耦校正的雷达协方差矩阵重构波束形成方法,其特征在于,在步骤7中,所述期望信号的最终导向矢量为 为入射方向为的信号导向矢量,为期望信号的最终入射方向;4. a kind of radar covariance matrix reconstruction beamforming method based on iterative mutual coupling correction as claimed in claim 3 is characterized in that, in step 7, the final steering vector of described desired signal is is the incident direction is The signal steering vector of , is the final incident direction of the desired signal; 所述均匀圆阵的自适应波束形成器的权矢量w,其表达式为:The weight vector w of the adaptive beamformer of the uniform circular array, its expression is: 其中,上标-1表示求逆操作,上标H表示共轭转置操作。Among them, the superscript -1 represents the inverse operation, and the superscript H represents the conjugate transpose operation.
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